Abstract (data abstract)

Diboson production in association with jets is studied in the fully leptonic final states, $\textrm{pp} \to (\textrm{Z}/\gamma^*)(\textrm{Z}/\gamma^*)+\textrm{jets} \to 2\ell2\ell'+\textrm{jets}$, ($\ell,\ell' = \textrm{e}$ or $\mu$) in proton-proton collisions at a center-of-mass energy of 13 TeV. The data sample corresponds to an integrated luminosity of 138 fb$^{-1}$ collected with the CMS detector at the LHC. Differential distributions and normalized differential cross sections are measured as a function of jet multiplicity, transverse momentum $p_\textrm{T}$, pseudorapidity $\eta$, invariant mass and $\Delta\eta$ of the highest-$p_\textrm{T}$ and second-highest-$p_\textrm{T}$ jets, and as a function of invariant mass of the four-lepton system for events with various jet multiplicities. These differential cross sections are compared with theoretical predictions that mostly agree with the experimental data. However, in a few regions we observe discrepancies between the predicted and measured values. Further improvement of the predictions is required to describe the ZZ+jets production in the whole phase space.

Figure 7 (left)

Data from Figure 7 (left).

10.17182/hepdata.145862.v1/t1

Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system,...
Figure 7 (right)

Data from Figure 7 (right).

10.17182/hepdata.145862.v1/t2

Differential cross sections normalized to the fiducial cross section as a function of the number of jets with $p_T >...
Figure 8 (upper left)

Data from Figure 8 (upper left).

10.17182/hepdata.145862.v1/t3

Differential cross sections normalized to the fiducial cross section as a function of the $p_T$ of the highest-$p_T$ jet
Figure 8 (upper right)

Data from Figure 8 (upper right).

10.17182/hepdata.145862.v1/t4

Differential cross sections normalized to the fiducial cross section as a function of the $p_T$ of the second-highest-$p_T$ jet
Figure 8 (lower left)

Data from Figure 8 (lower left).

10.17182/hepdata.145862.v1/t5

Differential cross sections normalized to the fiducial cross section as a function of the $|\eta|$ of the highest-$p_T$ jet
Figure 8 (lower right)

Data from Figure 8 (lower right).

10.17182/hepdata.145862.v1/t6

Differential cross sections normalized to the fiducial cross section as a function of the $|\eta|$ of the second-highest-$p_T$ jet
Figure 9 (left)

Data from Figure 9 (left).

10.17182/hepdata.145862.v1/t7

Differential cross sections normalized to the fiducial cross section as a function of the pseudorapidity difference between the two highest-$p_T$...
Figure 9 (right)

Data from Figure 9 (right).

10.17182/hepdata.145862.v1/t8

Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the two highest-$p_T$...
Figure 10

Data from Figure 10.

10.17182/hepdata.145862.v1/t9

Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system,...
Figure 11 (upper left).

Data from Figure 11 (upper left).

10.17182/hepdata.145862.v1/t10

Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...
Figure 11 (upper right).

Data from Figure 11 (upper right).

10.17182/hepdata.145862.v1/t11

Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...
Figure 11 (lower left).

Data from Figure 11 (lower left).

10.17182/hepdata.145862.v1/t12

Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...
Figure 11 (lower right).

Data from Figure 11 (lower right).

10.17182/hepdata.145862.v1/t13

Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...
Figure 12 (upper left).

Data from Figure 12 (upper left).

10.17182/hepdata.145862.v1/t14

Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...
Figure 12 (upper right).

Data from Figure 12 (upper right).

10.17182/hepdata.145862.v1/t15

Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...
Figure 12 (lower left).

Data from Figure 12 (lower left).

10.17182/hepdata.145862.v1/t16

Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...
Figure 12 (lower right).

Data from Figure 12 (lower right).

10.17182/hepdata.145862.v1/t17

Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...

Figure 7 (left)

Figure 7 (right)

Figure 8 (upper left)

Figure 8 (upper right)

Figure 8 (lower left)

Figure 8 (lower right)

Figure 9 (left)

Figure 9 (right)

Figure 10

Figure 11 (upper left).

Figure 11 (upper right).

Figure 11 (lower left).

Figure 11 (lower right).

Figure 12 (upper left).

Figure 12 (upper right).

Figure 12 (lower left).

Figure 12 (lower right).

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